Titlebook: New Challenges in Superconductivity: Experimental Advances and Emerging Theories; Proceedings of the N J. Ashkenazi,Mikhail V. Eremin,Fulin

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Flirtatious

Lattice Dynamics and Electron Pairing in High Temperature Superconductors, enhanced near the anti-nodal region and in the superconducting state, i.e. as the superconducting gap opens up. This unusual behavior is direct evidence that the electron-phonon interaction is correlated with the electron pairing in the high temperature superconductivity.

CON

Direct Arpes and TC Enhancement in Compressively Strained LSCO-214 Films,nd remaining ≈30meV below E. measured on unstrained samples. The associated reduction of the density of states does not diminish the superconductivity; rather, T. is strongly enhanced (up to factor of two) in compressively strained thin films.

半球

ASTER

椭圆

Pseudogap Behavior in Underdoped Cuprates,havior for the uniform magnetic susceptibility found in the underdoped cuprates and use this to propose a physical picture of the underdoped cuprates and to estimate the fraction of quasiparticles that become superconducting in underdoped superconductors.

Flu表流动

呼吸

Sum Rules and Energy Scales in BiSrCaCuO,c energy decreases in the superconducting state, unlike in conventional BCS superconductors. As a consequence, the Ferrell-Glover-Tinkham sum rule is not satisfied up to this energy scale. This stands as a very unconventional behavior, contrasted with the overdoped Bi-2212 sample.

享乐主义者

Nuclear Spin Relaxation and Incommensurate Magnetism in Doped Cuprates,s new result substitutes for a “pseudogap” regime in a broad class of high-. cuprates and stems from the 1st order phase transition that starts well above the superconductivity . but becomes frustrated because of broken electroneutrality in the CuO. plane.

considerable

Two Fluids Formation in the Normal State of High-, Superconductor,er, TEP shows deviation from the linear-. dependence at a certain temperature ., which is consistent with the pseudogap temperature. The systematic change of the TEP behavior is discussed in terms of the two fluids model of bound pairs and independent normal carriers.